Q: The instantaneous gas discharge of the system and the C-E

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The discussion revolves around the concept of mass conservation in a closed system, particularly when air is expelled. Participants clarify that while the mass of the entire system remains constant, the mass within the control volume can change over time due to the flow of air. The equations presented illustrate how the mass flow rate is related to the density and velocity of the expelled air. There is a distinction made between the system as a whole and the control volume, emphasizing that the system includes all mass entering, exiting, or accumulating within the control volume. Overall, the conversation highlights the complexities of fluid dynamics and mass conservation principles.
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Homework Statement
Confusing in the conservation of mass.
Relevant Equations
Continuity Equation
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Q: Why is air expelled from the system, yet the system's mass remains unchanged? Isn't mass related to volume?
 

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The system includes the expelled air.
 
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If the system includes air output, how should the cross-section be determined?
In a closed system, isn't it the case that fluids cannot cross the system boundaries? However, the following equation is indeed correct.
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Frabjous said:
The system includes the expelled air.
 
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tracker890 Source h said:
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If the system includes air output, how should the cross-section be determined?
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The system is the total mass. It's not changing in time. The tank is the control volume. The portion of the systems mass inside the control volume is changing in time, so you get:

$$ \frac{d}{dt} \int_{cv} \rho ~d V \llap{-} = - \int_{cs} \rho \vec{V} \cdot d \vec{A} $$

which reduces to ( uniformily distributed properties):

$$ \frac{d}{dt} m_{cv} = - \rho_e A_e V_e $$
 
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tracker890 Source h said:
Q: Why is air expelled from the system, yet the system's mass remains unchanged? Isn't mass related to volume?
Could you please explain why you are taking the time derivative of a 4-dimensional volume integral?

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berkeman said:
Could you please explain why you are taking the time derivative of a 4-dimensional volume integral?

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I was going to mention there are one too many integral signs. 😬
 
erobz said:
The system is the total mass. It's not changing in time. The tank is the control volume. The portion of the systems mass inside the control volume is changing in time, so you get:

$$ \frac{d}{dt} \int_{cv} \rho ~d V \llap{-} = - \int_{cs} \rho \vec{V} \cdot d \vec{A} $$

which reduces to ( uniformily distributed properties):

$$ \frac{d}{dt} m_{cv} = - \rho_e A_e V_e $$
So, my thoughts are as follows, is this correct?
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berkeman said:
Could you please explain why you are taking the time derivative of a 4-dimensional volume integral?

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Accidentally typed the wrong characters, it has been corrected.
 
tracker890 Source h said:
So, my thoughts are as follows, is this correct?
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Yeah, that's how you are to look at it. That first derivative being non-zero is not something you are going to encounter when it comes to mass as the property in R.T.T.

In essence the system is not the control volume, its "the stuff" moving through the control volume, be it mass, momentum , or energy. The "system" enters the control volume, exits the control volume, and/or accumulates within the control volume.
 
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erobz said:
Yeah, that's how you are to look at it. That first derivative being non-zero is not something you are going to encounter when it comes to mass as the property in R.T.T.

In essence the system is not the control volume, its "the stuff" moving through the control volume, be it mass, momentum , or energy. The "system" enters the control volume, exits the control volume, and/or accumulates within the control volume.
Thank you for the detailed and patient explanation. ^^
 
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